We synthesized polycrystalline perovskite-type Lii o n -c o n d u c t i n g o x i d e s ( g e n e r a l f o r m u l a : A B O 3 ) , Sr 0.5−x Li 0.3+2x Ti 0.3 Ta 0.7 O 3 (x = 0.030−0.100), and assessed their crystal structure, microstructure, ionic conductivity, and electrochemical stability. Based on first-principles calculations, local structure changes accompanied by Li-ion diffusion were discussed. It was found that the average structure of Sr 0.5−x Li 0.3+2x Ti 0.3 Ta 0.7 O 3 (x = 0.030−0.100) is a cubic perovskite-type one, and at x = 0.042, i.e., Sr 0.458 Li 0.384 Ti 0.3 Ta 0.7 O 3 , the highest bulk ionic conductivity and the total ionic conductivity at 300 K were observed to be 1.87 × 10 −3 and 1.05 × 10 −3 S cm −1 , respectively, which are greater than those of La 2/3−x Li 3x TiO 3 (LLTO). The first-principles calculations suggested that BO 6 octahedra are distorted, and the Li-ion diffusion is assisted by the dynamic distortion of BO 6 octahedra coupled with the second-order Jahn−Teller effect. The reduction potential of Sr 0.458 Li 0.384 Ti 0.3 Ta 0.7 O 3 was 1.6−1.7 V vs Li/Li + , which is comparable to that of LLTO. A cell using a Sr 0.458 Li 0.384 Ti 0.3 Ta 0.7 O 3 pellet with a deposited thin film LiCoO 2 cathode on one side was successfully operated as a secondary battery at room temperature, indicating that the compound can be applied as a solid electrolyte for Li-ion batteries.